Pseudo-Zernike polynomials

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In mathematics, pseudo-Zernike polynomials are well known and widely used in the analysis of optical systems. They are also widely used in image analysis as shape descriptors.

Definition

They are an orthogonal set of complex-valued polynomials defined as

Vnm(x,y)=Rnm(x,y)ejmarctan⁡(yx),

where x2+y2≤1,n≥0,|m|≤n and orthogonality on the unit disk is given as

∫02π∫01r[Vnl(rcos⁡θ,rsin⁡θ)]∗×Vmk(rcos⁡θ,rsin⁡θ)drdθ=πn+1δmnδkl,

where the star means complex conjugation, and r2=x2+y2, x=rcos⁡θ, y=rsin⁡θ are the standard transformations between polar and Cartesian coordinates.

The radial polynomials Rnm are defined as[1]

Rnm(r)=∑s=0n−|m|Dn,|m|,s rn−s

with integer coefficients

Dn,|m|,s=(−1)s(2n+1−s)!s!(n−|m|−s)!(n+|m|−s+1)!.

Examples

Examples are:

R0,0=1

R1,0=−2+3r

R1,1=r

R2,0=3+10r2−12r

R2,1=5r2−4r

R2,2=r2

R3,0=−4+35r3−60r2+30r

R3,1=21r3−30r2+10r

R3,2=7r3−6r2

R3,3=r3

R4,0=5+126r4−280r3+210r2−60r

R4,1=84r4−168r3+105r2−20r

R4,2=36r4−56r3+21r2

R4,3=9r4−8r3

R4,4=r4

R5,0=−6+462r5−1260r4+1260r3−560r2+105r

R5,1=330r5−840r4+756r3−280r2+35r

R5,2=165r5−360r4+252r3−56r2

R5,3=55r5−90r4+36r3

R5,4=11r5−10r4

R5,5=r5

Moments

The pseudo-Zernike Moments (PZM) of order n and repetition l are defined as

Anl=n+1π∫02π∫01[Vnl(rcos⁡θ,rsin⁡θ)]∗f(rcos⁡θ,rsin⁡θ)rdrdθ,

where n=0,…∞, and l takes on positive and negative integer values subject to |l|≤n.

The image function can be reconstructed by expansion of the pseudo-Zernike coefficients on the unit disk as

f(x,y)=∑n=0∞∑l=−n+nAnlVnl(x,y).

Pseudo-Zernike moments are derived from conventional Zernike moments and shown to be more robust and less sensitive to image noise than the Zernike moments.[1]

See also

References

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